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The Dirac operators $$ Ly = i 1 & 0 0 & -1 \frac{dy}{dx} + v(x) y, \quad y =y_1 y_2, \quad x\in[0,\pi],$$ with $L^2$-potentials $$ v(x) = 0 & P(x) Q(x) &0,  \quad P,Q \in L^2 ([0,\pi]), $$ considered on $[0,\pi]$ with periodic,antiperiodic or Dirichlet boundary conditions $(bc)$, have discrete spectra,and the Riesz projections $$ S_N = \frac{1}{2\pi i} \int_{|z|= N-{1/2}}(z-L_{bc})^{-1} dz, \quad P_n = \frac{1}{2\pi i} \int_{|z-n|= {1/4}}(z-L_{bc})^{-1} dz $$ are well--defined for $|n| \geq N$ if $N $ issufficiently large. It is proved that $$\sum_{|n| > N} \|P_n - P_n^0\|^2 <\infty, $$ where $P_n^0, n \in \mathbb{Z},$ are the Riesz projections of thefree operator.  Then, by the Bari--Markus criterion, the spectral Riesz decompositions  $$ f = S_N f + \sum_{|n| >N} P_n f, \quad \forall f \in L^2; $$ convergeunconditionally in $L^2.$

Bari-Markus property for Riesz projections of 1D periodic Dirac operators